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Unimon qubit

Superconducting qubits seem promising for useful quantum computers, but the currently wide-spread qubit designs and techniques do not yet provide high enough performance. Here, we introduce a superconducting-qubit type, the unimon, which combines the desired properties of increased anharmonicity, fu...

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Detalles Bibliográficos
Autores principales: Hyyppä, Eric, Kundu, Suman, Chan, Chun Fai, Gunyhó, András, Hotari, Juho, Janzso, David, Juliusson, Kristinn, Kiuru, Olavi, Kotilahti, Janne, Landra, Alessandro, Liu, Wei, Marxer, Fabian, Mäkinen, Akseli, Orgiazzi, Jean-Luc, Palma, Mario, Savytskyi, Mykhailo, Tosto, Francesca, Tuorila, Jani, Vadimov, Vasilii, Li, Tianyi, Ockeloen-Korppi, Caspar, Heinsoo, Johannes, Tan, Kuan Yen, Hassel, Juha, Möttönen, Mikko
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group UK 2022
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9653402/
https://www.ncbi.nlm.nih.gov/pubmed/36371435
http://dx.doi.org/10.1038/s41467-022-34614-w
Descripción
Sumario:Superconducting qubits seem promising for useful quantum computers, but the currently wide-spread qubit designs and techniques do not yet provide high enough performance. Here, we introduce a superconducting-qubit type, the unimon, which combines the desired properties of increased anharmonicity, full insensitivity to dc charge noise, reduced sensitivity to flux noise, and a simple structure consisting only of a single Josephson junction in a resonator. In agreement with our quantum models, we measure the qubit frequency, ω(01)/(2π), and increased anharmonicity α/(2π) at the optimal operation point, yielding, for example, 99.9% and 99.8% fidelity for 13 ns single-qubit gates on two qubits with (ω(01), α) = (4.49 GHz, 434 MHz) × 2π and (3.55 GHz, 744 MHz) × 2π, respectively. The energy relaxation seems to be dominated by dielectric losses. Thus, improvements of the design, materials, and gate time may promote the unimon to break the 99.99% fidelity target for efficient quantum error correction and possible useful quantum advantage with noisy systems.